/*===================================================================*/
 /* NRDF D1833 Data No.3                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 D#=D1833;
 TITLE=/ Neutron-production double-differential cross sections of
         iron and lead by 0.8 and 1.5 GeV protons in the most-forward
         direction /;
 ATH=(D.SATOH'1', N.SHIGYO'1', K.ISHIBASHI'1', Y.TAKAYAMA'1',
      S.ISHIMOTO'1', Y.IWAMOTO'1', H.TENZOU'1', T.NAKAMOTO'2',
      M.NUMAJIRI'2', S.MEIGO'3');
 INST-ATH=(2JPNKYU'1', 2JPNKEK'2', 2JPNJAE'3');
      /* '1' Department of Applied Quantum Physics and Nuclear
              Engineering */
 REF=NST;
 VLP=40(2003)283;
 /* Secondary reference 
    - NSTS, 4(2004)14 (N.Shigyo et al., Preliminary data given)
 RCTS=(FE(P,N)X, PB(P,N)X);
 PHQS=ENGY-SPEC;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,3;
 /* 2003-08-12 : Compiled+Checked, Im. */
 /* 2005-02-08 : Received, On. Received by e-mail from N.Shigyo */
 /* 2010-02-23 : Altered, Nf. REFERENCE: NSTS added */
 PHQ=ENGY-SPEC;
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'5';
 /* '5' 12-GeV PS */
 INST-ACC=2JPNKEK;
 POL-PRJ=0%;
 ION-SOURCE=/ Spallation (Incident protons were generated as secondary
              particles from an internal target which was placed in the
              12-GeV PS main ring.) /;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'6',TOF'7');
 /* '6' NE102A scintillator was mounted as a veto detector to
        reject the charged particle events. */
 /* '7' The high-resolution TOF measurement of 0-degree neutron was
        done. This provides a higher detection efficiency and uses a
        simpler data analysis than the recoil proton method. */
 ERS-DET=150MEV'8';
 /* '8' for 800 MeV protons */
 EFCN-DET=/ The neutron detection efficiencies were obtained from
            calculation results of SCINFUL-QMD [D.Satoh, et al., IEEE
            Trans. Nucl. Sci., 48, 1165 (2001); D.Satoh, et al., J.
            Nucl Sci. Technol., Supplement 2, 657 (2002)]. /;
 ANL=(INCASC'9',INCASC'10');
 /* '9' NMTC/JAM[K.Niita et al., JAERI-Data/Code 2001-007, JAERI,
        (2001).] */
 /* '10' JQMD[K.Niita et al., JAERI-Data/Code 99-042, JAERI,
         (1999).] */
 /* 2010-02-23 : Altered, Nf. STATUS: Free text revised */
 RCT=FE(P,N)X;
 THK-TGT=XMG/CM**2'18';
 /* '18' 30 mm */
 INC-ENGY-LAB-RANGE=1.5GEV;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,3;
 SYS-ERR=15%'11';
 /* '11' Ambiguity of neutron detection efficiency */
 INC-ENGY-LAB=1.5GEV;
 THTL=0DEG;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE'19' FLAG'20'
 (MEV) (MB/SR/MEV) (MB/SR/MEV) (NODIM)
 400.00 1.3735 +-0.27471 1.
 450.00 1.3430 +-0.26860 1.
 500.00 1.1952 +-0.23903 1.
 550.00 1.0583 +-0.21165 1.
 600.00 1.0773 +-0.21547 X
 650.00 1.0140 +-0.20280 X
 730.00 1.0467 +-0.19350 X
 850.00 1.3961 +-0.24323 X
 1000.0 1.3841 +-0.26483 X
 1150.0 0.85948 +-0.16384 X
 1300.0 0.52730 +-0.11019 X
 1450.0 0.33300 +-0.062260 X
 1600.0 0.18762 +-0.048086 X
 \END;
 /*===================================================================*/